Communication
[
34]
1
also be facilely modulated. In this work, using quaternary am-
with similar structures. The lower O quantum yield of Ru1
2
II
monium-modified bipyridine as ligand, three new Ru com-
may result from its shorter excited state lifetime.
plexes Ru1–Ru3 with four, six, and eight positive charges
Antibacterial performances of the complexes against S.
aureus and MRSA are presented in Figure 2. In the dark, all ex-
amined complexes did not affect the growth of S. aureus (Fig-
(
Figure 1) were easily prepared. The spherical octahedral coor-
II
dination structure and hydrophilic cationic character of the Ru
core may distinguish them from the reported organic aPDT
ure 2B). Upon light irradiation at 470 nm for 20 min (LED,
À2
2
2.5 mWcm ), Ru1–Ru3 showed concentration-dependent
bactericidal effect against S. aureus (Figure 2a). At 15 mm, Ru3
led to a colony-forming unit (CFU) reduction of 6.87 log units,
much higher than Ru1 (4.15 log units) and Ru2 (4.10 log units).
The CFU reduction can be directly observed on 3m Petrifilm
2
+
Aerobic Count Plates (Figure S6). In sharp contrast, Ru(bpy)3
exhibited negligible antibacterial activity in the same condi-
tions, demonstrating the key roles of the peripheral positive
charges. Obviously, more positive charges that Ru1–Ru3 bears
facilitate their binding toward negatively charged S. aureus,
1
and improve bioavailability of O .
2
It is worth noting that complex Ru3 exhibited remarkable
photoinactivation capability against MRSA. As shown in Fig-
ure 2C, the CFU reduction by Ru3 (15 mm) was still as high as
Figure 1. Chemical structures of complexes Ru1, Ru2, and Ru3.
5
.75 log units. We also compared the anti-MRSA performance
[
14–23]
agents,
which generally have large planar conjugated and
of Ru3 with that of traditional antibiotics, methicillin and van-
comycin (Figure 2D). As expected, MRSA showed resistance to
methicillin, but was eradicated effectively by vancomycin. At
10 mm of vancomycin, a CFU reduction of 5.89 log units was
observed. The comparable bactericidal ability of Ru3 demon-
strates again the important role of the peripheral positive
charges that a Ru complex takes, which transforms a totally
II
highly hydrophobic skeletons, making these Ru complexes ef-
ficiently bind to bacteria but not mammalian cells. Our results
indicate that complex Ru3 bearing eight positive charges ex-
hibited the most potent aPDT activity against S. aureus, includ-
ing MRSA. Notably, all three complexes showed extremely low
toxicity toward mammalian cells even upon visible light irradia-
tion, indicative of their high selectivity.
2
+
inert [Ru(bpy)3] to a highly potent aPDT agent.
The detailed synthesis and structure characterization of the
complexes Ru1–Ru3 may be found in Supporting Information
Complexes Ru1–Ru3 can also inactivate E. coli under light ir-
radiation, but with less efficiency (Figure S7). The dense and
compact outer membranes of E. coli may hamper the photo-
damage from Ru1–Ru3. Interestingly, complex Ru2 displayed
the highest photoinactivation effect, the reason is unknown
yet.
(
[
SI). The normalized absorption and emission spectra of
2
+
Ru(bpy)3]
(abbreviated as Ru0) and Ru1–Ru3 in PBS are
shown in Figure S4 (SI). Ru1–Ru3 display redshifted MLCT
metal to ligand charge transfer) absorption and emission com-
(
pared with that of Ru0. The introduction of electron-withdraw-
ing bpy-TMEDA ligand in Ru1–Ru3 will lower the energy level
of p*(bpy-TMEDA)-based LUMO (lowest unoccupied molecular
orbital) more efficiently than that of t (Ru)-based HOMO (high-
Besides CFU measurements, we also examined the morpho-
logical changes of bacteria by SEM (Figure 3). S. aureus cells
(2 mL) in the exponential phase were harvested, 1 mL of which
was treated with Ru3 and then exposed to light irradiation.
The untreated S. aureus cells maintained their morphology in-
tegrity. However, the aPDT treated cells showed damaged and
deformed cell walls, and the leakage of intracellular compo-
nents may partially account for the death of S. aureus. The re-
sults suggest that the cell wall might be the target of Ru3,
which is in good agreement with the expected strong electro-
static attraction between highly positively charged aPDT
agents and highly negatively charged bacterial surfaces.
The binding/uptake of the complexes Ru1–Ru3 by bacterial
cells was measured with Inductively Coupled Plasma Mass
Spectrometric (ICP-MS). Bacteria suspension was incubated in
the dark in the presence of Ru complexes (10 mm) for 40 min.
After centrifugation to remove the supernatant, Ru content
was measured by ICP-MS. As shown in Table 1, the uptake in-
creased with the increase of positive charges from Ru1 to Ru3.
For complex Ru3, the binding/uptake level was measured to
2g
est occupied molecular orbital), thus leading to redshifted
MLCT absorption and emission. Similar results were also report-
II
ed for other electron-withdrawing groups modified Ru com-
[
30,31]
plexes.
With the number of bpy-TMEDA ligand increasing
from Ru1 to Ru3, the energy level of HOMO will be stabilized
further, whereas that of LUMO will be less affected, thus a
blueshifted emission is observed from Ru1 to Ru3. Similar to
1
their parent complex Ru0, whose O quantum yield in H O is
2
1
2
[
32]
0
.41, Ru1–Ru3 can also generate O efficiently. Using 3,3’-
2
1
(
anthracene-9,10-diyl)-dipropanoic acid (9,10-ADPA) as O trap-
2
[
33]
1
ping agent, which reacts with O in a quantitative fashion
2
1
to produce a non-absorbing/emitting compound, the O2
quantum yields were measured to be 0.32Æ0.03 for Ru1,
0
.40Æ0.05 for Ru2 and 0.38Æ0.04 for Ru3 in H O by monitor-
2
ing the absorption decay of 9,10-ADPA at 378 nm (Figure S5).
The luminescence lifetimes in H O were measured to be
2
8
5
66 ns for Ru0, 282 ns for Ru1, 517 ns for Ru2 and 847 ns for
be around 25 ng Ru/10 cells at the dose of 10 mm, consistent
with the antibacterial activity. z-potential measurements are in
II
Ru3, which is consistent with other reported Ru complexes
&
&
Chem. Eur. J. 2019, 25, 1 – 7
2
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